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Self-Assembled Bismuth Selenide (Bi2se3) Quantum Dots Grown by Molecular Beam Epitaxy

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Self-Assembled Bismuth Selenide (Bi2se3) Quantum Dots Grown by Molecular Beam Epitaxy City University of New York (CUNY) CUNY Academic Works Publications and Research City College of New York 2019 Self-assembled Bismuth selenide (Bi2se3) quantum dots grown by molecular beam epitaxy Marcel S. Claro CUNY City College Ido Levy CUNY City College Abhinandan Gangopadhyay Arizona State University David J. Smith Arizona State University Maria C. Tamargo CUNY City College How does access to this work benefit ou?y Let us know! More information about this work at: https://academicworks.cuny.edu/cc_pubs/710 Discover additional works at: https://academicworks.cuny.edu This work is made publicly available by the City University of New York (CUNY). Contact: [email protected] www.nature.com/scientificreports OPEN Self-assembled Bismuth Selenide (Bi2Se3) quantum dots grown by molecular beam epitaxy Received: 5 September 2018 Marcel S. Claro 1,5, Ido Levy1,2, Abhinandan Gangopadhyay3, David J. Smith4 & Accepted: 28 January 2019 Maria C. Tamargo1,2 Published: xx xx xxxx We report the growth of self-assembled Bi2Se3 quantum dots (QDs) by molecular beam epitaxy on GaAs substrates using the droplet epitaxy technique. The QD formation occurs after anneal of Bismuth droplets under Selenium fux. Characterization by atomic force microscopy, scanning electron microscopy, X-ray difraction, high-resolution transmission electron microscopy and X-ray refectance spectroscopy is presented. Raman spectra confrm the QD quality. The quantum dots are crystalline, with hexagonal shape, and have average dimensions of 12-nm height (12 quintuple layers) and 46-nm width, and a density of 8.5 × 109 cm−2. This droplet growth technique provides a means to produce topological insulator QDs in a reproducible and controllable way, providing convenient access to a promising quantum material with singular spin properties. Te electronic confnement in all three dimensions of semiconductor quantum dots (QDs) leads to unique quan- tum properties. A discrete energy spectrum is produced, and the confnement impacts how the electrons interact with each other and to external infuences, such as electric and magnetic felds. Tese quantum efects can be tuned by changes in the sizes of the dots or the strength of the confning potential. Such QDs are used in many diverse applications, spanning from devices such as lasers1, solar cells2 and photodetectors3, to the study of new physical phenomena, such as single photon interactions4 and spin manipulation5. In the well-known common semiconductors, QDs are typically created using heterostructures defined by lithography or by self-assembled crystal growth. QD growths by molecular beam epitaxy (MBE) in Stranski-Krastanov mode6 and by droplet epitaxy7,8 are the most commonly used techniques for Si-Ge, and III-V semiconductors. QDs could also be formed by the electrostatic confnement of 2D electron gases9. However, in materials where the electronic states are protected by time-reversal symmetry, i.e., Graphene10, and the class of materials known as Topological Insulators (TI), the electrostatic potential cannot confne or scatter electrons as usual, a property known as the Klein paradox11. Tus, quantum confnement in these materials can normally only be achieved by the formation of 0D nanostructures. Tree-dimensional TIs, such as Bi2Se3 and related materials, are insulators in the bulk form, usually with a narrow band gap. However, they have surface states with spins that are locked with momentum and protected by time-reversal symmetry12. Tin flms possess favorable bulk to surface volume ratio to enhance the TI properties and have applications that include quantum computing, dissipation-less electronics, spintronics, enhanced ther- 12 moelectric efects and high performance fexible photonic devices . Among the many TIs, Bi2Se3 is particularly interesting because its band gap is larger than those of most other TIs, and the experimentally verifed Dirac cone is at the gamma point13. Tese materials exhibit a tetradymite crystal structure with Se-Bi-Se-Bi-Se units, 14 commonly referred to as quintuple layers, that are bonded together by van der Waals forces . Bi2Se3 can be syn- thetized as bulk crystals, thin flms or nanoparticles by several methods15. Bulk crystals have been synthetized by Bridgman–Stockbarger16, fux17 and other methods, and then chemically or mechanically exfoliated to study their properties as thin flms18. Excellent results have been achieved this way. Unfortunately, these methods have poor controllability and low yield, and cannot be applied for large-scale production or large-area applications. Solution-based processes have also been applied successfully to synthesize nanoparticles and to study their novel 1Department of Chemistry, The City College of New York, New York, NY, 10031, USA. 2Ph.D. Program in Chemistry, The Graduate Center of the City University of New York, New York, NY, 10016, USA. 3School for Engineering of Matter, Transport and Energy, Arizona State University, Tempe, AZ, 85287, USA. 4Department of Physics, Arizona State University, Tempe, AZ, 85287, USA. 5INL – International Iberian Nanotechnology Laboratory, 4715-330, Braga, Portugal. Correspondence and requests for materials should be addressed to M.C.T. (email:[email protected] ) SCIENTIFIC REPORTS | (2019) 9:3370 | https://doi.org/10.1038/s41598-019-39821-y 1 www.nature.com/scientificreports/ www.nature.com/scientificreports Figure 1. Spotty (1 × 1) RHEED pattern observed afer formation of Bi2Se3 QDs. Te inset illustrates the steps involved in the growth sequence. optical properties, from photothermic absorption19 to nonlinear optical properties such as saturable absorbers, which have applications in photonics20. Te chemical vapor deposition (CVD) method can produce relatively high quality nanomaterials on a large scale15. However, none of these methods can achieve the purity and con- trollability of MBE14. In MBE the material grows in ultra-high vacuum using only fuxes of high purity Bi and 21 Se. High quality Bi2Se3 has been grown successfully by MBE on diferent substrates and, due to the ability to controllably dope materials achieved with MBE, the Quantum Anomalous Hall efect could be observed22. Additionally, MBE-grown QDs can be readily incorporated into multilayers and heterostructures with other TIs23 as well as with 3D materials24, thus greatly expanding the range of possibilities for novel physical phenomena and device applications. As with other materials, we expect that some properties of TIs and Bi2Se3, especially those related to spintronic and quantum computing, can be enhanced by quantum dot confnement25–27. In lithographically defned QDs, the quantum confnement was already previously demonstrated28. However, to our knowledge, very few experi- ments have been done to investigate the efect of the quantum confnement of TIs. Te lack of adequate means to fabricate mesoscopic structures in a reproducible, high purity and controlled way is identifed as a major obstacle. 29 Nonetheless, the MBE growth of Bi2Se3 occurs by van der Waals epitaxy since it is a layered material, and strain cannot be used to induce QD formation by the Stranski-Krastanov mode as in other materials. In this work we demonstrate a viable method to create self-assembled quantum dots of Bi2Se3 by molecular beam epitaxy based on the droplet epitaxy technique. Results and Discussion Te samples were grown in a dual-chamber Riber 2300P system equipped with in situ refection high-energy electron difraction (RHEED). Te GaAs semi-insulating (001) substrates were prepared by oxide desorption in the frst chamber, followed by the growth of 200 nm of GaAs at 575 °C by conventional MBE. Te substrates were cooled under an overpressure of Arsenic and a fat c(4 × 4) surface reconstruction, typical of As-terminated GaAs, was observed by RHEED at the end of this process. Te substrates were then moved under ultra-high vacuum (UHV) to the second chamber for growth of the Bi droplets and the QDs. Te background pressure of the sec- ond chamber, where the droplet and QD growth occurred, was 1–4 × 10−10 Torr during growth. High-purity 6N bismuth (Bi) and selenium (Se) were provided by a RIBER double-zone cell for Bi and a Riber VCOR cracker cell for Se. Fluxes were measured by an ion gauge placed in the path of the fuxes. Te estimated fux ratio was 10:1 Se −8 to Bi. Te temperature used for the Bi source was 730 °C and the beam equivalent fux (BEP) was 2 × 10 Torr. Tese conditions led to an average growth rate of 32 nm/h for Bi2Se3 by van der Waals epitaxy. Te growth of the bismuth droplets was initiated by opening the Bi shutter when the prepared substrate tem- perature reached 250 °C, and the fat c(4 × 4) surface reconstruction was still visible. During the frst few minutes, a circular ring started to appear in the RHEED pattern and the streaky pattern from GaAs began to fade, indicat- ing the formation of amorphous material on the surface. Te RHEED pattern became totally difuse afer 15 min with barely visible spots that appeared in some orientations. For the droplet sample, the Bi shutter was closed at that time and the sample was cooled down and extracted for analysis. For QD formation, afer the Bi shutter closure, the Se shutter was opened and the sample was exposed to Se fux at the same temperature of 250 °C. Te RHEED pattern changed from the difuse pattern to a “spotty” (1 × 1) reconstruction pattern. Afer approx. 2 mins, the RHEED pattern was totally transformed into the pattern shown in Fig. 1. Te droplets were exposed to the Se fux for 40 min in total to ensure the complete formation of the Bi2Se3 and to minimize Se vacancies. However, since the RHEED was stable afer the frst few minutes of growth, it should be possible to reduce this time considerably in future studies. Te inset in Fig. 1 illustrates the steps that occur during the QD growth. SCIENTIFIC REPORTS | (2019) 9:3370 | https://doi.org/10.1038/s41598-019-39821-y 2 www.nature.com/scientificreports/ www.nature.com/scientificreports Figure 2.
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